Telescópios:
Radiotelescópios
Prof. Jorge Meléndez
Os principios básicos de radio astronomia foram
apresentados no seminário do Jullian. A seguir informações
complementares sobre o tema.
The radio region
The radio region observable from Earth occupies a wide range within
the electromagnetic spectrum.
The wavelength region in which Earth-based radio astronomy can be pursued comprises wavelengths 15 (or 20) m - 1 mm. This corresponds to frequencies of between (15) 20 MHz and 300 GHz.
H2O Reflected
or
Porque demorou tanto?
Astrônomos sabiam demais …
Em ondas de rádio:
Replacing
the
exponential term
in
Planck's equation
by its
Taylor-series
approximation
Inicio da radioastronomia
Natural radio emission from our Galaxy was detected accidentally in 1932 by Karl Guthe Jansky, a physicist working as a radio engineer for Bell Telephone Laboratories.
Karl Jansky (1905-1950) and the antenna that discovered cosmic
radio static at 20.5 MHz. It rotated in
azimuth on four wheels scavenged from a Ford Model T. An accurate replica of this antenna is located at the NRAO in Green Bank, WV.
The New York Times of May 5, 1933
''New Radio Waves
Traced to Centre of the
Milky Way.''
Astronomers ignored this
discovery, because they
couldn’t understand how
that strong emission was
possible. Se fosse de origem
térmica, corresponderia a
Grote Reber's backyard radio telescope in Wheaton, IL. The parabolic reflector is about 10 m in diameter.
Only Grote Reber took Jansky's discovery
seriously. He was an amateur radio operator and professional radio engineer.
Em 1937 observou em 3300 MHz,
mas teve insucesso.
Grote Reber (22 dec 1911 – 20 dec 2002)
In 1938 he finally succeeded in
detecting and mapping (with about
10 degree angular resolution) the
Galaxy at 162 MHz, confirming
Jansky's discovery and
demonstrating that the radio
emission has a distinctly
nonthermal spectrum
http://www.cv.nrao.edu/course/astr534/Discovery.html
Henry Ford: o insucesso é apenas uma oportunidade
para recomeçar de novo
3300 MHz: nada
910 MHz: nada
Reber, G. 1940
(ApJ, 91, 621).
The radio sky
Céu em radio
(4.85 GHz) desde
Green Bank
Seen here is the radio sky over the
telescopes of the National Radio Astronomy Observatory in
Green Bank, VA. Note the shell-like
supernova remnants and irregularly shaped star formation regions. The point-like objects are not stars but
mostly distant radio galaxies.
htt p://w w w .c v. nra o.edu /c o urs e/ a s tr5 34 /T o ur .ht m l
The Sun at
4.6 GHz
http://metsahovi.aalto.fi/en/research/projects/solar_radio/mapping_tracking/
13.7m diameter radio telescope at Metsähovi, Kylmälä
Radio receiver for Planck CMB from Planck, an ESA mission
http://www.cea.inpe.br/roi/
Zonas de Silêncio
http://www.cea.inpe.br/roi/arquivos/ZonaSilencio_v2.pdf
Região de Atibaia. Ponto branco no meio é o observatório. O círculo maior é a zona de silêncio (R ~ 2 km). As elipses menores são regiões de desmatamento e degradação florestal. As maiores fontes de interferência são fornos de microondas, controles remotos, redes de alta tensão, walk talks, acionadores de lâmpadas
fluorescentes,
computadores e torres de celular.
http://www2.jpl.nasa.gov/magellan/
Venus by Magellan
(radar)
Animation of the variation of the synchrotron emission at 1400 MHz from Jupiter (VLA
observations) with a computer model (Levin et al. 2001, Geophys. Res. Lett., 28,903) using an assumed electron distribution and magnetic field. The model simulates ground based radio observations well. The thermal emission from Jupiter has been subtracted, and representative magnetic field lines are shown. The animation covers one rotation of Jupiter, frames are 20 degrees apart in central longitude. The animation shows the East West asymmetry of the emitted radiation in the equatorial plane. The "wobble" of the emitted radiation is due to the misalignment of the rotation pole of Jupiter and the magnetic pole.
h tt p :/ /ju n o .w isc .ed u /scie n ce_ma g n e tosphe re .html
http:// asd .gsfc. na sa.g ov/a rchi ve/a rcad e/scie nce _g al a xy .html
Mapa da galáxia em
408 MHz
The Galaxy in the 21cm line (1420.4 MHz) of neutral H. Red indicates directions of high HI column density, while blue and black show areas with little hydrogen
This false-color image of CO (J = 2-1) emission from the face-on spiral galaxy M51 was made with the Smithsonian Submillimeter Array (SMA). It reveals regions
containing dense molecular gas, dust, and star formation that are optically obscured.
Cassiopeia A (Cas A)
is the remnant of a supernova explosion that occured over 300 years ago in our Galaxy, at adistance of about 11,000 light years from us. Its name is derived from the constellation in which it is seen:
Cassiopeia, the Queen. A radio supernova is the explosion that
occurs at the end of a massive star's life, and Cas A is the expanding shell of material that remains from such an explosion. This composite image is based on VLA data at three
different frequencies: 1.4, 5.0, and 8.4 GHz. The material that was ejected from the supernova
explosion can be seen in this image as bright filaments.
A high-resolution VLA image of the radio source Cygnus A. The bright central component is thought to coincide with a supermassive black hole that accelerates the relativistic electrons along two jets
terminating in lobes well outside the host galaxy.
The WMAP 7-year total-intensity image of the CMB. The intensity range is only 200uK
Pospelov & Pradler 2010 ARNPS 60, 539 Big Bang Nucleosynthesis as a Probe of New Physics
http://keckobservatory.org/news/international_team_on_keck_observatory_strengthens_big_bang_theory
Keck media release:
6/6/2013
“Back in 2004 HIRES was upgraded with CCDs having smaller pixels, allowing to see finer details in the spectrum,” University of Sao Paulo’s Jorge Meléndez said. “A high spectral resolution provided by HIRES is needed to study with exquisite detail the line profile and to estimate the presence of Lithium-6. The large light-collecting power of Keck Observatory allowed us to observe stars with a more ‘pristine’ composition than any previous study.”
SETI
Allen telescope array 350 dishes
(6m each)
Only 42 completed in 2007
(hibernation in April – Dec 2011 due
to lack of funds)
Wide field 2.45° at λ = 21 cm. Instantaneous frequency coverage from 0.5 to 11.2 GHz Arecibo
Resolução angular
⇨
Se λ = 0.1m e D = 7m,
= 1
o
●
Rádiotelescópios são limitados pela difração
⇨
(lembrando...) os ópticos são limitados pelo seeing
= 1.22
λ /d
λ (radio range observable from
Smith
No geral radiotelescópios não produzem imagens (detetores são
unidimensionais)
“Imageamento”
O rádio telescópio é um telescópio
com um “CCD” de um único pixel.
É necessário varrer a
região a ser observada.
Mas alguns rádio telescópios têm alimentadores múltiplos (Um CCD de mais de um pixel): O rádio telescópio de Parkes, 64 m, usa um receptor de 13 alimentadores em 21 cm, e o Five College
Radio Astronomy Observatory, 14 m, usa um receptor de 32 alimentadores no milimétrico!
Elementos de um radiotelescópio
Prato
+
Antena
+
sistema de
detecção
www.das.inpe.br
Feixe de entrada é plano-paralelo. Figura não está correta.Prato: focaliza a radiação na antena
Rádiotelescópios não precisam ter superficies continuas
36
36
Rádiotelescópios tem f/# baixo
Baixa f/# ajuda a proteger do ruído
O rádio telescópio de Cambridge, com f/<1 e D=32m.
Podem ser off-focus (asimetricos,
e.g. seção de parábola)
• Green bank Radiotelescope, 100x110m (F=60m), largest
steerable in the world (situated in West Virginia, USA)
64-metre Parkes radio telescope in Australia.
The dish surface was physically upgraded by adding smooth metal plates to the central part to provide focusing capability for centimetre and millimetre length
Effelsberg 100-m Radio Telescope
Max Planck Institute for Radio Astronomy (Bonn)
- Located in a valley to minimize intereference - Accuracy of the mirror surface better than 1mm
Interferometria
BDA
10 antenas. 25 m cada.
Separação de 8600 km. 1,2-96 GHz.